US8779995B2 - High-frequency waveguide and phase shifter using same, radiator, electronic device which uses this phase shifter and radiator, antenna device, and electronic device equipped with same - Google Patents

High-frequency waveguide and phase shifter using same, radiator, electronic device which uses this phase shifter and radiator, antenna device, and electronic device equipped with same Download PDF

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US8779995B2
US8779995B2 US13/122,270 US200913122270A US8779995B2 US 8779995 B2 US8779995 B2 US 8779995B2 US 200913122270 A US200913122270 A US 200913122270A US 8779995 B2 US8779995 B2 US 8779995B2
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Prior art keywords
waveguide
ridge
frequency
conductors
phase shifter
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US13/122,270
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US20110187614A1 (en
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Hideki Kirino
Isao Yamamoto
Masashi Watanabe
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Panasonic Corp
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Panasonic Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/18Phase-shifters
    • H01P1/182Waveguide phase-shifters
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/03Details of HF subsystems specially adapted therefor, e.g. common to transmitter and receiver
    • G01S7/032Constructional details for solid-state radar subsystems
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P3/00Waveguides; Transmission lines of the waveguide type
    • H01P3/12Hollow waveguides
    • H01P3/123Hollow waveguides with a complex or stepped cross-section, e.g. ridged or grooved waveguides
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/27Adaptation for use in or on movable bodies
    • H01Q1/32Adaptation for use in or on road or rail vehicles
    • H01Q1/3208Adaptation for use in or on road or rail vehicles characterised by the application wherein the antenna is used
    • H01Q1/3233Adaptation for use in or on road or rail vehicles characterised by the application wherein the antenna is used particular used as part of a sensor or in a security system, e.g. for automotive radar, navigation systems
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q1/00Details of, or arrangements associated with, antennas
    • H01Q1/27Adaptation for use in or on movable bodies
    • H01Q1/32Adaptation for use in or on road or rail vehicles
    • H01Q1/325Adaptation for use in or on road or rail vehicles characterised by the location of the antenna on the vehicle
    • H01Q1/3291Adaptation for use in or on road or rail vehicles characterised by the location of the antenna on the vehicle mounted in or on other locations inside the vehicle or vehicle body
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q13/00Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
    • H01Q13/10Resonant slot antennas
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/0006Particular feeding systems
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/06Arrays of individually energised antenna units similarly polarised and spaced apart
    • H01Q21/061Two dimensional planar arrays
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q3/00Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system
    • H01Q3/26Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture
    • H01Q3/30Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array
    • H01Q3/32Arrangements for changing or varying the orientation or the shape of the directional pattern of the waves radiated from an antenna or antenna system varying the relative phase or relative amplitude of energisation between two or more active radiating elements; varying the distribution of energy across a radiating aperture varying the relative phase between the radiating elements of an array by mechanical means
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/93Radar or analogous systems specially adapted for specific applications for anti-collision purposes
    • G01S13/931Radar or analogous systems specially adapted for specific applications for anti-collision purposes of land vehicles
    • G01S2013/9327Sensor installation details
    • G01S2013/93271Sensor installation details in the front of the vehicles
    • G01S2013/9375

Definitions

  • the present invention relates to a high-frequency waveguide and a phase shifter in which this is used, to a radiator, to an electronic device in which this phase shifter and radiator are used, and to an antenna device and an electronic device equipped with this.
  • a high-frequency waveguide used as a transmission path for high-frequency energy is constituted by combining first and second waveguide constituting bodies.
  • first and second waveguide constituting bodies each provided with a groove are integrated in a state in which the openings of the grooves are aligned, which constitutes a high-frequency waveguide.
  • Patent Literature 1 Japanese Laid-Open Patent Application 2004-48486.
  • Patent Literature 1 Japanese Laid-Open Patent Application 2004-48486
  • Patent Literature 2 Japanese Laid-Open Patent Application 2002-223113
  • the problem with the above prior art was that high-frequency energy leaked from the high-frequency waveguide.
  • the above-mentioned first and second waveguide constituting bodies are such that flanges provided around the outside of their grooves are integrated by welding or fastened with screws. If a gap should be formed in this process during a work error, then high-frequency energy will end up leaking from that portion.
  • the present invention employs a structure having a ridge in the middle of what is known as a waffle iron structure, equipped with first and second conductors and columnar protrusions.
  • the first and second conductors are disposed facing each other at a spacing of less than ⁇ 0 /2, where the free space wavelength of the operating frequency of a high-frequency signal is ⁇ 0 .
  • the ridge protrudes from one of the first and second conductors toward the other in a waveguide formation portion formed between the first and second conductors, and is formed extending along the waveguide formation portion.
  • a plurality of the columnar protrusions have a height of ⁇ 0 /4 and are disposed at a spacing of less than ⁇ 0 /2, on at least one of the first and second conductors on the outside of the waveguide formation portion and to the outside of the ridge.
  • a ridge is provided that protrudes from one of the first and second conductors toward the other in a waveguide formation portion formed between the first and second conductors, and is formed extending along the waveguide formation portion. Consequently, an electric field is concentrated between this ridge and the conductors facing it, and high-frequency energy moves in a direction perpendicular to this electric field, that is, in the lengthwise direction of the ridge. As a result, leakage of high-frequency energy outside the waveguide formation portion is much less likely to occur.
  • a plurality of columnar protrusions with a height of ⁇ 0 /4 are disposed at a spacing of less than ⁇ 0 /2 on at least one of the first and second conductors on the outside of the waveguide formation portion and to the outside of the ridge. Consequently, since a plurality of columnar protrusions are provided as mentioned above to the waveguide formation portion to the outside of this ridge, even if high-frequency energy should move to the outside of the ridge, movement of the high-frequency energy to the outside of the waveguide formation portion can be prevented. As a result, leakage of high-frequency energy can be effectively prevented.
  • Radar devices have come to be installed in automobiles in recent years for the purpose of collision avoidance, lane distance control, and so forth. These radar devices can take measurements even when the automobile is going around a curve, so a detection angle of about 15 degrees to the left and right (a total of 30 degrees) is needed.
  • One way to obtain this detection angle has been to use a configuration in which an antenna body is disposed in front of a transceiver via a waveguide body, and the antenna body is made movable to the left and right with respect to the waveguide body.
  • Patent Literature 2 Japanese Laid-Open Patent Application 2002-223113
  • the antenna apparatus ended up being bulky. Specifically, to obtain the above-mentioned large detection angle of about 15 degrees to the left and right with an antenna apparatus, the antenna body must be extremely large. An antenna apparatus including a configuration in which such a large antenna body is driven to the left and right ends up being quite bulky when its movable space is included.
  • the present invention comprises an antenna body, a stationary waveguide body, a movable waveguide body, and a transceiver.
  • the antenna body has first and second radiation element groups having radiation element rows including a plurality of radiation elements disposed at a specific spacing.
  • the movable waveguide body forms a waveguide body between itself and the stationary waveguide body, and moves relatively with respect to the stationary waveguide body.
  • the transceiver is provided to the rear of the antenna body, via the waveguide body.
  • the plurality of waveguides provided to the movable waveguide body has a first waveguide, a second waveguide, and a third waveguide.
  • the first waveguide is constituted by a plurality of waveguides corresponding to the first radiation element group.
  • the second waveguide is constituted by a plurality of waveguides corresponding to the second radiation element group.
  • the third waveguide is such that the phase difference in the first and second radiation element groups between the radiation element rows of the first radiation element group and the radiation element rows of the second radiation element group, which are adjacent to one another, is matched to be the same as the phase difference between the mutually adjacent other radiation element rows included in the first and second radiation element groups.
  • the antenna body is a stationary type
  • the waveguide body disposed to its rear is a movable type, which allows a wider detection angle to be obtained. Accordingly, the size is much smaller than when the antenna body itself is made movable within the apparatus.
  • the constitution of the above-mentioned first, second, and third waveguides shortens the distance between the first and second radiation element groups to be about the same as the distance between adjacent transmission and reception openings. Thus, this prevents the scattering of radio waves in unnecessary directions, which increases as the distance grows between the first and second radiation element groups.
  • FIG. 1 is an oblique view of an automobile to which an embodiment of the present invention has been applied;
  • FIG. 2 is an oblique view of the antenna apparatus pertaining to an embodiment of the present invention
  • FIG. 3 is an exploded oblique view of the antenna apparatus pertaining to an embodiment of the present invention.
  • FIG. 4 is a cross section of a basic waveguide pertaining to an embodiment of the present invention.
  • FIG. 5 is an oblique view of a basic waveguide pertaining to an embodiment of the present invention.
  • FIG. 6 is an oblique view of a waveguide having a through-hole pertaining to an embodiment of the present invention.
  • FIG. 7 is an oblique view of a phase shifter in an embodiment of the present invention.
  • FIG. 8 is a cross section of a laminated type of variable phase shifter pertaining to an embodiment of the present invention.
  • FIG. 9 is a cross section of a laminated type of fixed phase shifter pertaining to an embodiment of the present invention.
  • FIG. 10 is an oblique view of a sixth plate body as seen from the rear;
  • FIG. 11 is an oblique view of a fifth plate body as seen from the rear;
  • FIG. 12 is an oblique view of a fifth plate body as seen from the front;
  • FIG. 13 is an oblique view of a fourth plate body as seen from the rear;
  • FIG. 14 is an oblique view of a fourth plate body as seen from the front;
  • FIG. 15 is an oblique view of a third plate body as seen from the rear;
  • FIG. 16 is an oblique view of a third plate body as seen from the front;
  • FIG. 17 is an oblique view of a second plate body as seen from the rear;
  • FIG. 18 is an oblique view of a second plate body as seen from the front;
  • FIG. 19 is an oblique view of a first plate body as seen from the front;
  • FIG. 20 is an exploded oblique view of a fourth plate body
  • FIG. 21 is a layout diagram of the phase shifter of a beam variable antenna pertaining to an embodiment of the present invention.
  • FIG. 22 is a phase relation diagram for a beam variable antenna pertaining to an embodiment of the present invention.
  • FIG. 23 is an oblique view of a high-frequency waveguide in which the ridge height is variable periodically;
  • FIG. 24 is a wavelength graph of a high-frequency waveguide in which the ridge height is variable periodically;
  • FIG. 25 is an oblique view of a radiator that makes use of a high-frequency waveguide in which the ridge height is variable periodically;
  • FIG. 26 is a directionality graph when the distance between radiation elements is varied
  • FIG. 27 is a layout diagram for a phase shifter of a beam variable antenna pertaining to an embodiment of the present invention.
  • FIGS. 28 a and 28 b are a side cross section and a plan view of a plate body, illustrating a configuration in which the dimensions (height and width) in the lengthwise direction of the ridge pertaining to another embodiment of the present invention are varied.
  • 1 is an automobile body, and four tires 2 are provided under this automobile body 1 .
  • These tires 2 are rotationally driven by an engine (not shown) installed under a hood 3 of the automobile body 1 .
  • a panel (not shown) for controlling the operation of the tires 2 is provided within the vehicle interior 4 .
  • the antenna apparatus 6 shown in FIG. 2 is provided above a bumper 5 on the front face side of the automobile body 1 .
  • radio waves of 76.5 GHz are emitted from the front face side of the automobile body 1 , over left and right ranges (such as 15 degrees, or a total of 30 degrees) horizontally from the center with respect to the forward range (such as 150 meters), while the angle thereof is successively scanned back and forth.
  • the antenna apparatus 6 receives reflected waves from up to 150 meters ahead at the angle at which the waves were emitted, so that any objects (such as other automobiles, debris, or the like that is ahead) and so forth are detected within a range of 150 meters ahead, and this information is used for various controls over the automobile body 1 .
  • this can be control in which debris is detected in the road ahead, and a warning is given in the interior 4 , for example.
  • the antenna apparatus 6 shown in FIG. 2 is constituted by various parts as shown in FIG. 3 .
  • the orientation of the parts in FIG. 3 corresponds to that in FIGS. 1 and 2 .
  • 7 is an antenna body, and a transceiver 9 is disposed to the rear of this antenna body 7 via a waveguide body 8 . Also, a cover (a radio wave-transmissible cover) 10 is disposed in front of the antenna body 7 , and a case 11 is disposed to the rear of the transceiver 9 .
  • the antenna body 7 is made up of two plate-like members comprising a plate body 12 and a plate body 13 .
  • the waveguide body 8 is made up of five plate-like members comprising the plate body 13 , a plate body 14 , a plate body 15 , a plate body 16 , and a plate body 17 .
  • the transceiver 9 is made up of a substrate base 18 , a controller 19 , and an RF circuit board 20 .
  • the reason that the plate body 13 is included in both the antenna body 7 and the waveguide body 8 is that the front side of the plate body 13 is used as the antenna body 7 , while the rear side is used as the waveguide body 8 .
  • the plate bodies 12 , 13 , 14 , 15 , 16 , and 17 are each provided with columnar protrusions, ridges, and through-holes (for interlayer connection) as discussed below (see FIGS. 10 to 19 ).
  • the plate bodies 12 and 13 of the antenna body 7 , as well as the plate bodies 14 , 15 , 16 , and 17 of the waveguide body 8 are maintained in a state of being separated at a specific spacing.
  • the plate body 15 of the waveguide body 8 has a disk shape, and is configured such that the plate body 14 and the plate body 16 move rotationally with a specific spacing between them, around the center of the disk. Consequently, the desired detection angle can be ensured to the left and right merely by rotationally driving the disk-shaped plate body 15 . Since there is no need for the antenna body to be made movable as in the past, the configuration can be simplified.
  • the phase shifter and the high-frequency waveguide are constituted inside the antenna body 7 and the waveguide body 8 so that even in a state in which the above-mentioned plate bodies 12 to 17 are separated by a specific gap, the high-frequency energy supplied from the transceiver 9 will not be scattered in the surroundings, but will be phase controlled and allocated by an antenna plate 12 .
  • FIG. 4 is a cross section illustrating the basic operating principle of the high-frequency waveguide and the phase shifter, while FIG. 5 is an oblique view thereof.
  • the high-frequency waveguide in this embodiment is formed by two conductors disposed in parallel at a spacing of less than ⁇ 0 /2 (where ⁇ 0 is the free space wavelength of the operating frequency of a high-frequency signal), that is, a lower conductor 22 (first conductor, second conductor) and an upper conductor 23 (second conductor, first conductor).
  • the high-frequency waveguide has a so-called waffle iron structure, in which columnar protrusions 24 (protrusions for preventing electromagnetic wave leakage) with a height of approximately ⁇ 0 4/ are disposed two-dimensionally on the surface of the lower conductor 22 (one of the conductors) at a spacing of ⁇ 0 /2 between each other.
  • a ridge 25 formed continuously along the transmission path of high-frequency energy is provided on the inside of this waffle iron structure.
  • the ridge 25 is provided to a waveguide formation portion between the lower conductor 22 and the upper conductor 23 .
  • a plurality of the columnar protrusions 24 are provided on the outside of this ridge 25 and on the outside of the waveguide formation portion.
  • the two conductors 22 and 23 disposed in parallel at a spacing of less than ⁇ 0 /2 operate as a parallel plate waveguide that transmits only a basic mode having only a perpendicular electric field to the conductors.
  • the gaps between the columnar protrusions 24 are equivalent to a transmission path whose distal ends have been short-circuited by the lower conductor 22 .
  • the region of the gaps between the columnar protrusions 24 in a plane 26 that connects the distal ends of the columnar protrusions 24 with a height of ⁇ 0 /4 as shown in FIG. 4 is equivalent to a magnetic wall with which an electric field cannot be present in a direction perpendicular to this plane.
  • the structure in FIGS. 4 and 5 is inherently a parallel plate waveguide that can transmit high-frequency energy (radio waves) resulting from an electric field perpendicular to the two conductors 22 and 23 .
  • a waffle iron structure in which the columnar protrusions 24 with a height of ⁇ 0 /4 are disposed two-dimensionally a characteristic is that high-frequency energy cannot be transmitted.
  • the reason for specifying the gap between the columnar protrusions 24 to be less than ⁇ 0 /2 is to prevent a higher-order transmission mode from occurring in the gaps between the columnar protrusions 24 , and reliably obtain the characteristic whereby high-frequency energy cannot be transmitted.
  • the structure shown in FIGS. 4 and 5 functions as a basic waveguide capable of efficiently transmitting high-frequency energy along the ridge, without scattering it to the surroundings.
  • the proportion of voltage and current in the transmitted high-frequency energy can be varied by varying the height in the lengthwise direction of the ridge 25 (see FIG. 23 ), or by varying the width in a direction perpendicular to the lengthwise direction (see FIG. 28 ).
  • impedance paths of difference characteristics can be produced. That is, if the width is varied or the height is varied in the lengthwise direction of the ridge 25 , the size of the capacity component (C) formed between the conductor 23 and the opposing ridge 25 can be varied. As a result, impedance paths of difference characteristics can be easily produced.
  • a branched line can also be easily produced by dividing the ridge 25 into a plurality of segments in its extension direction (more specifically, into a T shape) (see FIG. 11 ).
  • the high-frequency waveguide of this embodiment is used in an antenna feeder circuit with numerous couplings or branches, such as a milliwave on-board radar, both production and assembly will be simple, with no worry about poor contact due to aging, and a low-loss antenna apparatus can be obtained.
  • FIG. 6 shows a structure in which through-holes 27 a and 27 b are provided in a direction perpendicular to the waveguide formation portion in order to use the above-mentioned high-frequency waveguide in laminated form.
  • 27 a and 27 b are through-holes through which the high-frequency energy leaves and enters the upper and lower layers
  • 28 is a choke structure for efficiently transmitting high-frequency energy to the through-holes 27 a and 27 b as well as blocking the transmission of high-frequency energy in the direction in which the ridge 25 extends.
  • This structure comprises a waveguide with an open distal end of ⁇ R /4 (where ⁇ R is the wavelength of a radio wave that transmits the waveguide formation portion from the ends of the through-holes 27 a and 27 b , and a plurality of columnar protrusions 24 with a height of approximately ⁇ 0 /4 disposed on the outside of the waveguide in which said distal end is opened.
  • a position where there has been movement to a length of ⁇ R /4 of the waveguide with the opened distal end is equivalent with a short-circuited state. Accordingly, the waveguide wall of the through-hole 27 is short circuited with the ridge 25 . Thus, high-frequency energy is efficiently transmitted from the ridge 25 to the through-hole 27 .
  • the columnar protrusions 24 with a height of ⁇ 0 /4 disposed on the outside of the waveguide with the opened distal end reduce leakage from the distal end of the waveguide, and are provided to achieve a more ideal open state.
  • FIG. 7 shows a structure in which the shape of the through-hole to the upper layer on one side of the ridge 25 has been designed such that a waveguide is obtained even if the lower conductor 22 and the upper conductor 23 should slide relative to each other.
  • 27 a and 27 b are through-holes through which the high-frequency energy leaves and enters the upper and lower layers
  • 29 is a choke structure provided to the upper conductor 23 to efficiently transmit high-frequency energy to the through-hole 27 b as well as blocking the transmission of high-frequency energy in the direction in which the ridge 25 extends.
  • This choke structure 29 is such that a plurality of waveguide-shaped grooves, which have a depth of approximately ⁇ W /4 and which are short-circuited at the distal ends, are disposed, with the ⁇ R /4 position at the front, where ⁇ R is the wavelength on the waveguide from the end of the through-hole 27 b to the upper layer.
  • ⁇ W the in-guide wavelength of the groove at the waveguide formation portion.
  • the entrance to waveguide-shaped grooves provided to the upper conductor 23 having a depth of approximately ⁇ W /4 and which are short-circuited at the distal ends, is equivalent to an open state. Accordingly, return current is blocked at the lower face of the upper conductor 23 that makes a pair with the current flowing over the ridge 25 at this position, and the impedance is open at this position.
  • the through-hole 27 b provided at a position of ⁇ R /4 from this position, the ridge and the waveguide wall of the through-hole 27 b is equivalent to a short circuit. As a result, high-frequency energy is efficiently transmitted from the ridge 25 to the through-hole 27 b.
  • the reason for disposing a plurality of waveguide-shaped grooves which have a depth of approximately ⁇ W /4 and which are short-circuited at the distal ends is to suppress the leakage of current that jumps out of the waveguide-shaped grooves, and achieve a more ideal open state.
  • phase shifter in this embodiment, the features of the high-frequency waveguide shown in FIG. 6 are retained. Consequently, the high-frequency energy is not scattered to the surroundings, and coupling between adjacent phase shifters can also be kept low. Furthermore, production and assembly will be simple, with no worry about poor contact due to aging. In particular, a low-loss phase shifter can be realized in the milliwave band of an onboard radar or the like.
  • phase shifter Next, a specific example of a phase shifter will be described, corresponding to a description using the actual drawings discussed below.
  • FIG. 8 shows a cross section of a structure in which two of the phase shifters shown in FIG. 7 are used, and lower conductors 22 a and 22 b of the two phase shifters are laminated back to back, wherein this structure is cut along ridges 25 a and 25 b .
  • the upper and lower conductors 23 a and 23 b are fixed to each other, and an intermediate conductor in which the conductors 22 a and 22 b are integrated is slid in the direction of the arrow 30 in the drawing. Consequently, the waveguide length between through-holes 27 ba and 27 bb (between A-A) varies via through-holes 27 aa and 27 ab (linking path).
  • the structure operations as a variable phase shifter that varies the phase of high-frequency energy passing between A-A. That is, the phase shifter in FIG. 8 is distinguished from the phase shifter in FIG. 7 in that the positions of the two input/output terminals (the through-holes 27 ba and 27 bb ) of the phase shifter indicated by A in FIG. 8 do not vary during operation of the phase shifter, and that the phase shift is twice the amount of relative sliding of the intermediate conductor.
  • FIG. 9 is a cross section of a structure in which two of the phase shifters shown in FIG. 7 are used, and lower conductors 22 a and 22 b of the two phase shifters are laminated back to back, wherein this structure is cut along ridges 25 a and 25 b .
  • the left and right orientation of the two phase shifters is the opposite of that in FIG. 8 . Consequently, even when the intermediate conductor is slid in the direction of the arrow 30 in the drawing, there is no change in the waveguide length between the through-holes 27 ba and 27 bb (between B-B) via the through-holes 27 aa and 27 ab (linking paths).
  • this structure can operate as a fixed phase shifter that does not change the phase of the high-frequency energy passing through B-B.
  • this can be used in application where the goal is to allow the high-frequency energy to pass through, but with no change in the phase, between the upper and lower conductors 23 a and 23 b.
  • phase shifter and high-frequency waveguide described above are used inside the waveguide body 8 and the antenna body 7 of the antenna apparatus 6 in this embodiment.
  • phase shifter having the structure shown in FIGS. 7 and 8 is used for a phase array antenna that has a plurality of phase shifters (such as an onboard radar) and with which the ratio of the amount of shift between the plurality of phase shifters is kept constant while the amounts are simultaneously varied
  • the constitution is as follows.
  • the lower conductor 22 and the upper conductor 23 are not slid directly, and a plurality of phase shifters in which the ridge 25 of FIG. 7 is arc-shaped are disposed in concentric circles with the same radius ratio, as shown in the detail diagrams of the plate bodies 12 to 17 , as discussed below.
  • a movable conductor plate (plate body 15 ) and stationary conductor plate (plate bodies 14 and 16 ) corresponding to the lower conductor 22 and upper conductor 23 in FIG. 7 are moved rotationally parallel to each other, with the rotational axis being the center of the concentric circles. That is, since the radius ratio of the ridges is constant, a phase shifter group is obtained with which the shift amounts are varied while a constant shift amount ratio is maintained with respect to a given rotational movement angle.
  • a waffle iron structure comprising columnar protrusions with a height of approximately ⁇ /4, and a waveguide comprising a ridge provided along the transmission path of high-frequency energy are used. Accordingly, the plate body 12 , the plate body 13 , even though the plate body 14 , the plate body 15 , the plate body 16 , and the plate body 17 do not come into physical contact, they are maintained in a state of being separated by a constant spacing, and there is no leakage of high-frequency energy to the surroundings. Also, the degree of coupling between adjacent lines or phase shifters is kept low. Thus, production and assembly will be simple, with no worry about poor contact due to aging.
  • a low-loss antenna can be realized in the milliwave band of an onboard radar or the like. Furthermore, with the antenna apparatus 6 in this embodiment, the fact that the plate bodies 12 to 17 are not in physical contact is taken advantage of so that the plate body 15 of the waveguide body 8 in particular is moved rotationally at a specific spacing with respect to the plate body 14 and the plate body 16 . Consequently, it is possible to realize a beam variable antenna that includes a phase shifter with a simple configuration.
  • high-frequency energy is sent once from the plate body 16 to the plate body 14 , passing through the plate bodies 12 to 17 . After this, it passes again through the plate bodies 14 and 15 and is returned to the plate body 16 . It then passes through the plate bodies 16 and 15 again and reaches the plate body 14 . Consequently, numerous phase shifters can be housed within a small area. This allows the overall size of the antenna apparatus 6 to be reduced.
  • FIG. 10 is an oblique view of the plate body 17 of the waveguide body 8 as seen from the rear.
  • the orientation display in the drawing corresponds completely to the orientation display in FIGS. 1 and 2 , and the same holds true for the oblique views of other plate bodies discussed below.
  • the high-frequency energy outputted from the transceiver 9 is inputted through a through-hole 31 into the interior of the waveguide body 8 .
  • the inputted high-frequency energy enters a ridge end 32 a of the plate body 16 in FIG. 11 , and is transmitted along the ridge 32 . It is then split into two branches, after which it enters through-holes 33 going to the front layer.
  • the structure shown in FIG. 6 is used for the path here from the through-hole 31 to the through-holes 33 .
  • the high-frequency energy that has entered the through-hole 33 comes out a through-hole 34 of the plate body 16 in FIG. 12 .
  • the shape of all of the through-holes between the layers discussed below, including the through-holes 33 and 34 is that of a double-ridge rectangular waveguide having ridges on the two long sides of a rectangular waveguide, rather than the rectangular waveguide shown in FIGS. 6 and 7 , so that high-frequency energy can be transmitted efficiently to the ridge of the upper and lower layers.
  • the through-holes of the phase shifter input and output components, including the through-hole 34 have a shape in which part of the short side of a rectangular waveguide bulges outward so as to conform to the ridge. A raised portion or cut-out is also provided to part of the ridge for conformity.
  • the high-frequency energy coming out of the through-hole 34 in FIG. 12 goes into the ridge 35 of the plate body 15 in FIG. 13 .
  • the energy is transmitted along the ridge 35 and enters a through-hole 36 going to the front layer.
  • the high-frequency energy that has entered the through-hole 36 goes out to the through-hole 37 in the plate body 15 in FIG. 14 .
  • the high-frequency energy that has gone out to the through-hole 37 is transmitted along the ridge and enters a through-hole 38 that goes through to the front layer of the plate body 14 in FIG. 15 .
  • the structure shown in FIG. 9 is used for the path that links the through-holes 34 , 36 , 37 , and 38 . Consequently, even if the plate body 15 moves rotationally with respect to the plate bodies 13 and 16 , there will be no change in the phase of the high-frequency energy from the through-holes 34 to 38 .
  • the high-frequency energy that has entered the through-hole 38 in FIG. 15 goes out to a through-hole 39 in the plate body 14 in FIG. 16 , after which it is transmitted along the ridge. It is then split into two branches, and enters through-holes 40 and 41 that lead to the rear layer.
  • the high-frequency energy inputted from the transceiver 9 to the through-hole 31 of the plate body 17 passes forward between the plate bodies 17 , 16 , and 15 and reaches the through-hole 39 in the plate body 14 . After this, it passes rearward between the plate bodies 14 and 15 again and returns to the plate body 16 , so the direction of progress of the high-frequency energy is reversed at the plate body 14 .
  • the high-frequency energy that enters the through-hole 40 comes out from a through-hole 42 in the plate body 14 in FIG. 15 .
  • the high-frequency energy that comes out of the through-hole 42 goes into a ridge 44 of the plate body 15 in FIG. 14 , is transmitted along the ridge 44 , and enters a through-hole 45 going to the rear layer.
  • the high-frequency energy that enters the through-hole 45 goes out into a through-hole 46 in the plate body 15 in FIG. 13 .
  • the high-frequency energy that comes out from the through-hole 46 is transmitted along a ridge 47 , and goes from the ridge 47 into a through-hole 48 going to the rear layer of the plate body 16 in FIG. 12 .
  • the structure shown in FIG. 9 is also used for the path that links the through-holes 42 , 45 , 46 , and 48 .
  • the high-frequency energy that has entered the through-hole 41 comes out from the through-hole 43 in the plate body 14 in FIG. 15 .
  • the high-frequency energy that has come out of the through-hole 43 goes into a ridge 49 of the plate body 15 in FIG. 14 , is transmitted along the ridge 49 , and enters a through-hole 50 going to the rear layer.
  • the high-frequency energy that has entered the through-hole 50 goes out to a through-hole 51 in the plate body 15 in FIG. 13 , is transmitted along a ridge 52 , and enters a through-hole 53 going to the rear layer of the plate body 16 in FIG. 12 .
  • the high-frequency energy that has entered the through-holes 48 and 53 shown in FIG. 12 comes out from the through-holes 54 and 55 , respectively, in the plate body 16 in FIG. 11 . After this, it is transmitted along ridges 32 b and 32 c , is split into four branches each, and enters through-holes 56 and 57 going to the front.
  • the high-frequency energy that has been outputted from the transceiver 9 passed forward through the plate bodies 17 , 16 , and 15 to reach the plate body 14 , and then passed rearward back through the plate bodies 15 , 16 , and 17 and returned to the plate body 16 once again passes through the plate bodies 16 , 15 , and 14 and reaches the plate body 14 , so the progress direction at the plate body 16 is reversed.
  • the high-frequency energy that has entered the through-holes 56 and 57 comes out from through-holes 58 and 59 in the plate body 16 in FIG. 12 . After this, the high-frequency energy enters positions 60 a and 61 a on ridges 60 and 61 of the plate body 15 in FIG. 13 , is transmitted over the four ridges 60 and 61 , and enters through-holes 62 and 63 going to the front.
  • the high-frequency energy that has entered the through-holes 62 and 63 goes out to through-holes 64 and 65 in the plate body 15 in FIG. 14 . After this, the high-frequency energy it is transmitted via the four ridges 66 and 67 and enters through-holes 68 and 69 going to the front layer of the plate body 14 in FIG. 15 from positions 66 a and 67 a on the ridges 66 and 67 .
  • the structure shown in FIG. 8 is used for the path that links the through-holes 58 , 62 , 64 , and 68 and the through-holes 59 , 63 , 65 , and 69 .
  • the high-frequency energy that has entered the through-holes 68 and 69 comes out from through-holes 70 and 71 in the plate body 14 in FIG. 16 . After this, it is transmitted over four ridges 72 and 73 , and enters through-holes 74 and 75 in the plate body 13 in FIG. 17 from positions 72 a and 73 a on the ridges 72 and 73 . The high-frequency energy further comes out from through-holes 76 and 77 in the plate body 13 in FIG. 18 .
  • the high-frequency energy that has come out from the through-holes 76 and 77 resonates on four ridges 78 and 79 , which are waveguides used to excite radiation elements.
  • the resonance current on the ridges 78 and 79 also resonates radiation element groups 12 a and 12 b formed on the plate body 12 in FIG. 19 .
  • the resonance magnetic flow of the radiation element groups 12 a and 12 b becomes a radiation source, and high-frequency energy is radiated toward the front space of the antenna apparatus 6 .
  • the flow of high-frequency energy that entered one of the through-holes 33 in FIG. 11 was described, but the high-frequency energy that enters the other through-hole 33 passes through the same path and is radiated toward the front space from radiation element groups 12 c and 12 d in FIG. 19 .
  • the radiation element group 12 and the radiation element group 12 b , and the radiation element group 12 c and the radiation element group 12 d form left and right symmetry in the shape of the phase shifters passed through. Accordingly, when the plate body 15 moves rotationally, the phase signs of the variable phase shifters have mutually opposing polarity.
  • the configuration comprises a combination of a plurality of transmission paths, including those with which the phase of high-frequency energy changes or does not change when the plate body 15 is moved rotationally with respect to the plate bodies 14 and 16 .
  • a plurality of arc-shaped phase shifters are disposed in concentric circles with the same radius ratio. Consequently, when the plate body 15 moves rotationally with respect to the plate bodies 14 and 16 , a phase difference can be generated that is proportional to the radius ratio of the phase shifters. Furthermore, as shown in FIG. 19 , a layout can be employed in which the density of radiation element rows 12 aa to 12 ad , 12 ba to 12 bd , 12 ca to 12 cd , and 12 da to 12 dd is raised in the left and right direction.
  • These radiation element rows 12 aa to 12 ad , 12 ba to 12 bd , 12 ca to 12 cd, and 12 da to 12 dd are a group of radiation elements constituted by disposing a plurality of radiation elements in the up and down direction.
  • the means for rotationally moving the plate body 15 is constituted by a disk-shaped plate body 80 , a position detection plate 81 , a clamping plate 82 , a screw 83 , and a motor 84 .
  • the motor 84 must be installed in a hole 85 in the center of the plate body 15 . Accordingly, there is a restriction in that a phase shifter cannot be disposed in the center of the disk-shaped plate body 80 .
  • phase shifter layout in this embodiment will now be described.
  • FIG. 21 is a diagram of the phase shifter layout in the antenna apparatus 6 pertaining to this embodiment (beam variable antenna), and FIG. 22 is a diagram of the phase relationships in the antenna apparatus 6 pertaining to this embodiment.
  • the antenna apparatus 6 of this embodiment has an input terminal 32 x and radiation element groups 12 a to 12 d .
  • the radiation element groups 12 a to 12 d correspond to slotted radiation element rows 12 aa to 12 ad , 12 ba to 12 bd , 12 ca to 12 cd , and 12 da to 12 dd , a plurality of which are arranged in the up and down direction.
  • FIGS. 21 and 22 the points corresponding to the through-holes 33 , 34 , 38 , 39 , 40 , 41 , 42 , 43 , 48 , 53 , 55 , 56 , 57 , 58 , 59 , 68 , 69 , 70 , and 71 that connect the above-mentioned plate bodies 12 to 17 are indicated with circles.
  • the lines corresponding to the high-frequency waveguides provided to the plate bodies 12 to 17 are indicated by the two solid lines 87 and 88 and the two dotted lines 89 and 90 .
  • the dotted line 89 indicates a high-frequency waveguide comprising a ridge provided to the rear of the plate body 16
  • the dotted line 90 indicates a high-frequency waveguide comprising a ridge provided to the front of the plate body 15
  • the solid line 87 indicates a high-frequency waveguide comprising a ridge provided to the rear of the plate body 15
  • the solid line 88 indicates a high-frequency waveguide comprising a ridge provided to the front of the plate body 15 .
  • arc-shaped solid lines shown on the inside indicate a high-frequency waveguide 87
  • arc-shaped solid lines shown on the outside indicate a high-frequency waveguide 88 .
  • the numbers 91 , 92 , 93 , and 94 in FIG. 22 indicate the phase shifters shown in FIG. 21 .
  • the notations on the phase shifters indicate the amount of change in waveguide length corresponding to the amount of movement of each phase shifter when the plate body 15 moves rotationally by ⁇ /2 in the arrow direction in FIG. 21 .
  • the radiation element rows 12 aa to 12 ad , 12 ba to 12 bd , 12 ca to 12 cd , and 12 da to 12 dd are shown in the same order of arrangement.
  • the phase shifters 93 and 94 in FIG. 22 here are variable phase shifters with which the amount of phase shift changes with the plate body 15 shown in FIG. 18 moves rotationally.
  • the phase shifters 91 and 92 are fixed phase shifters with which the amount of phase shift does not change even though the plate body 15 shown in FIG. 9 moves rotationally.
  • FIG. 21 the connection shapes of the high-frequency waveguides 87 and 88 of these two kinds of phase shifter are depicted so as to correspond to the shapes of the high-frequency energy paths A-A and B-B in FIGS. 8 and 9 .
  • the radius from the rotational movement center of the plate body 15 of the high-frequency waveguide of the phase shifter 93 is 4 ⁇ r as shown in FIGS. 21 and 22 .
  • the radius from the rotational movement center of the plate body 15 of the high-frequency waveguide of the phase shifters 94 is 4.5 ⁇ r, 5.5 ⁇ r, 6.5 ⁇ r, and 7.5 ⁇ r, respectively, in that order from the inside.
  • the amounts of change in the waveguide length of the phase shifters of radiation element rows 12 aa to 12 dd from the input terminal 32 x in FIG. 22 are summed up while taking into account the signs contributed by combination of the direction of rotational movement of ⁇ and the layout of the phase shifters 91 to 94 when the plate body 15 has moved rotationally by ⁇ /2
  • the difference in the amounts of change in waveguide length between the mutually adjacent radiation element rows 12 aa and 12 ab , the radiation element rows 12 ab and 12 ac , . . . the radiation element rows 12 db and 12 dc , and the radiation element rows 12 dc and 12 dd is ⁇ r ⁇ in every case, as follows.
  • Radiation element row 12 ba: ⁇ 0+4 ⁇ r ⁇ 7.5 ⁇ r ⁇ ⁇ 3.5 ⁇ r ⁇
  • the plurality of waveguides formed in the waveguide body 8 form a variable phase shifter with which the phase of transmitted radio waves varies, and a fixed phase shifter that imparts a fixed phase amount according to the fixed transmission path length, regardless of the movement of the plate body 15 , when the plate body 15 (a movable waveguide body) rotates (or moves rotationally) and moves relatively with respect to the plate body 14 , the plate body 16 , and the plate body 13 .
  • the plurality of waveguides of the waveguide body 8 form a first waveguide ( 95 in FIG. 27 ), a second waveguide ( 96 in FIG. 27 ), and a third waveguide ( 97 in FIG. 27 ).
  • the first waveguide is constituted by a plurality of waveguides corresponding to first radiation element groups 12 a and 12 b .
  • the second waveguide is constituted by a plurality of waveguides corresponding to second radiation element groups 12 c and 12 d .
  • the third waveguide matches the waveguide length difference between radiation element row 12 bd of the first radiation element group and the radiation element row 12 ca of the second radiation element group to ⁇ r* ⁇ (that is, the sum of ⁇ r and ⁇ ), which is the waveguide length difference between other adjacent radiation element rows.
  • phase difference between mutually adjacent radiation element rows among all of the radiation element rows 12 aa to 12 ad , 12 ba to 12 bd , 12 ca to 12 cd , and 12 da to 12 dd can be made uniform in all cases, so scattering of radio waves in unnecessary directions can be reduced.
  • the motor 84 must be installed in the center of the plate body 15 constituting a phase shifter. Accordingly, when there is a limitation in that a phase shifter cannot be disposed in the center, a variable phase shifter that varies the phase when the plate body 15 is moved rotationally is combined with a fixed phase shifter that does not vary the phase. Consequently, a phase difference that is the same as that between other adjacent radiation element rows can be imparted between the adjacent radiation element rows 12 bd and 12 ca among the radiation element rows 12 ba to 12 cd included in the radiation element groups 12 b and 12 c in FIG. 19 . Thus, it is possible to raise the gain of the antenna apparatus 6 .
  • An antenna apparatus was described above in which the scattering of radio waves in unnecessary directions in the left and right direction in FIG. 1 was reduced.
  • the present invention is not limited to this, however.
  • the antenna apparatus may be such that the scattering of radio waves in unnecessary directions in the up and down direction in FIG. 1 is reduced.
  • FIG. 23 is an oblique view of a high-frequency waveguide in which the height of a ridge 95 is varied periodically.
  • FIG. 24 is a wavelength graph for a high-frequency waveguide in which the height of the ridge is varied periodically.
  • FIG. 25 is an oblique view of a radiator that makes use of a high-frequency waveguide in which the height of the ridge is varied periodically.
  • FIG. 26 is a directionality graph when the distance between the radiation elements is changed.
  • the high-frequency waveguide shown in FIG. 23 has the same structure and shape as the high-frequency waveguide shown in FIG. 5 , except for the ridge 95 , whose height varies in the lengthwise direction.
  • the upper conductor is not shown for the sake of simplifying the description, but the high-frequency waveguide is constituted by two conductors, namely, the upper conductor 23 and the lower conductor 22 , just as in FIG. 5 .
  • the high-frequency waveguide shown in FIG. 23 is provided with notches (recesses) 96 in the ridge 95 at a period of less than ⁇ R /4, where ⁇ R is the wavelength on the high-frequency waveguide shown in FIG. 5 at the operating frequency. This allows the height of the ridge 95 in its lengthwise direction to be varied periodically.
  • FIG. 24 is a graph of the relation between the depth of the notches 96 and the wavelength on the high-frequency waveguide.
  • ⁇ 0 be the free space wavelength of the operating frequency
  • the ratio ⁇ g / ⁇ 0 of the wavelength ⁇ g on the high-frequency waveguide to the free space wavelength ⁇ 0 can be varied over a range of approximately 1.15 to 0.85.
  • the principle behind the ability to vary the wavelength on the high-frequency waveguide is that since the notches 96 act as a distal end short-circuit line in which the bottom faces of the notches serve as the short-circuit distal ends and the two opposing side faces on the inside of the notches serve as the transmission path for high-frequency energy propagated over the high-frequency waveguide, an equivalent impedance of the distal end short-circuit line corresponding to the depth of the notches 96 is inserted in series to the high-frequency waveguide as a distributed constant component.
  • FIG. 25 shows a radiator that makes use of a high-frequency waveguide in which the height is varied at a period of less than ⁇ R /4 in the lengthwise direction of the ridge 95 . This corresponds to removing one high-frequency waveguide on the plate body 13 in FIG. 18 and one radiation element row on the plate body 12 in FIG. 19 .
  • the high-frequency waveguide constituted by the ridge 95 is open at both ends.
  • the length thereof is an integer multiple of the wavelength ⁇ g on the high-frequency waveguide.
  • the high-frequency waveguide is in a resonant state, and resonance current flows over the ridge 95 .
  • Radiation element rows 112 aa to 112 aj are disposed at opposing positions (on the plate body 12 ) at places where the resonance current on the ridge 95 is at its maximum and where the resonance current has the same orientation.
  • high-frequency energy of the same phase and amplitude is radiated into space from all of the radiation element rows 112 aa to 112 aj .
  • the radiator in FIG. 25 operates as an array antenna having its main beam in the forward direction.
  • FIG. 25 shows a case in which 10 ⁇ g is the length of the high-frequency waveguide and there are ten radiation element rows, but an array antenna having its main beam in the forward direction can be similarly obtained as long as K is equal to or greater than the number of radiation elements, wherein K ⁇ g is the length of the high-frequency waveguide.
  • the spacing 97 between the mutually adjacent radiation element rows 112 aa to 112 aj is matched to the wavelength on the high-frequency waveguide.
  • FIG. 26 shows the directionality characteristics in the ZX plane of the radiator in FIG. 25.
  • 98 is the directionality characteristics when the distance 97 between radiation elements is 1.15 ⁇ 0
  • 99 is the directionality characteristics when the distance 97 between radiation elements is 0.85 ⁇ 0 .
  • the main beam is in the forward direction, that is, in a direction with an angle of 0°.
  • the distance between the radiation element rows 112 aa to 112 aj is greater than the free space wavelength ⁇ 0
  • the direction in which the high-frequency energy radiated into space from the radiation element rows 112 aa to 112 aj is within an angle of ⁇ 90°, generating a so-called grating lobe that scatters radio waves in unnecessary directions.
  • the directionality characteristics in FIG. 26 generate a corresponding grating lobe having gain on the same level as the main beam in a direction with an angle of ⁇ 60°.
  • ⁇ R be the wavelength on the high-frequency waveguide when no notches 96 are provided at the operating frequency
  • the wavelength on the high-frequency waveguide is varied by varying the height at a period of less than ⁇ R /4 in the lengthwise direction of the ridge 95 .
  • a radiator with suppressed generation of a grating lobe at the same level as the main beam, which would degrade recognition accuracy, can be realized for an onboard radar by using a high-frequency waveguide in which the wavelength is further varied for the feeder line of the radiator.
  • the amount of change in the phase of high-frequency energy passing through a high-frequency waveguide with a unit length can be varied by varying the wavelength on the high-frequency waveguide. Consequently, an effect is that using this as a phase adjustment line affords greater latitude in the layout of the antenna feeder line. It should go without saying that this effect is the scope encompassed by the present invention.
  • a radar for monitoring automobiles ahead was used as an example of an electronic device featuring the high-frequency waveguide pertaining to the present invention.
  • this radar may be used in heavy machinery and the like used at construction sites and so forth.
  • an electronic device featuring the high-frequency waveguide of the present invention in the heavy machinery itself as a radar for monitoring the surroundings. If this is done, then when a person is near the machinery, for example, the machinery operator will be alerted to exercise caution, and can halt the operation of the machinery. This makes it possible to improve the safety of heavy machinery that makes less noise.
  • the dimension in the height direction of the ridge 95 was used as an example of varying the ridge 95 in its lengthwise direction to form a high-frequency waveguide, but the present invention is not limited to this.
  • a high-frequency waveguide may be formed by using a ridge 195 having two different heights Z 1 and Z 2 .
  • a high-frequency waveguide may be formed by using a lower conductor (plate body 213 ) that includes a ridge 295 whose width varies in the lengthwise direction, and in which the spacing between adjacent columnar protrusions (protrusions for preventing the leakage of electromagnetic waves) is less than ⁇ 0 /2.
  • the present invention allows a reduction in size and a simplification of the configuration of an antenna, without moving the antenna itself, and is therefore expected to be very useful in its application to automobiles and so forth where there is a need for smaller size and lighter weight for the purpose of conserving energy.

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US20110187614A1 (en) 2011-08-04

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